2012
DOI: 10.1108/15736101211281632
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Fluid‐structure interaction computational analysis of a piston‐cylinder based blast‐wave‐mitigation concept

Abstract: Purpose -This paper aims to utilize purpose advanced fluid-structure interaction, non-linear dynamics, finite-element analyses in order to investigate various phenomena and processes accompanying blast wave generation, propagation and interaction and to assess the blast-wave-mitigation potential of a piston-cylinder assembly placed in front of the target structure. Design/methodology/approach -The employed computational methods and tools are verified and validated by first demonstrating that they can quite acc… Show more

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Cited by 13 publications
(9 citation statements)
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“…Details regarding the bi-phasic Friedlander pressuredependent function and physical character of its parameters can be found in our previous work. 65,66 As far as the boundary conditions for the Lagrangian part of the computational domain are concerned, the following two types were applied simultaneously: (a) to mimic the skull/spine pivot joint, a coupling is created using a set of nodes at the skull base and the associated reference node is kinematically constrained to form a revolute joint and (b) to mimic the effect of neck-support muscles, six axialtype connectors are placed between four couplings on the skull and the base of the neck (modeled as a set of four nodes fixed in space). Using the approach outlined in our prior work, 67 muscles are modeled as passive elastic elements and their elastic stiffness is set accordingly.…”
Section: Problem Formulationmentioning
confidence: 99%
“…Details regarding the bi-phasic Friedlander pressuredependent function and physical character of its parameters can be found in our previous work. 65,66 As far as the boundary conditions for the Lagrangian part of the computational domain are concerned, the following two types were applied simultaneously: (a) to mimic the skull/spine pivot joint, a coupling is created using a set of nodes at the skull base and the associated reference node is kinematically constrained to form a revolute joint and (b) to mimic the effect of neck-support muscles, six axialtype connectors are placed between four couplings on the skull and the base of the neck (modeled as a set of four nodes fixed in space). Using the approach outlined in our prior work, 67 muscles are modeled as passive elastic elements and their elastic stiffness is set accordingly.…”
Section: Problem Formulationmentioning
confidence: 99%
“…A detailed overview of both EOS for the air/detonation-products mixture, and their parameterization for the C-4 high explosive (HE) in the mine, can be found in our prior work. [26][27][28] Since the gaseous mixture has zero effective shear stiffness, shear stresses cannot develop as a result of shear strain, but can develop as a result of a gradient in flow velocity, i.e. shear strain rate.…”
Section: He Chargementioning
confidence: 99%
“…A detailed overview of both EOS for the air/detonation-products mixture, and their parameterization for the C-4 high explosive (HE) in the mine, can be found in our prior work. 2628…”
Section: Problem Formulation and Computational Analysismentioning
confidence: 99%
“…Equations ( 18) and ( 19), allow determination of U r for a given level of blast intensity. Hence, u p and p r ¼ p g can now be solved using equations ( 8) and (17). Implementation of the procedure described above yields p r ¼ p g ¼ p s and the associated reflection coefficient (p r /p s ) is 1.0 for a rigid structure of infinitesimal mass.…”
Section: Fully Supported Incident Blast Wave Casementioning
confidence: 99%
“…19 Within the third group of strategies, various physical phenomena and processes are utilized in order to lower the strength and increase the thickness of the blast-induced shock wave(s) within the target structure. For example: (i) in the case of polyurea blast wave mitigating coatings, shock wave energy dissipation is accomplished through activation of a secondorder rubbery-to-glassy phase transition under shock loading; 20,21 (ii) in the case of foam-like cellular material-based protective structures, shock energy is dissipated via the cell-wall buckling and cell-wall/cell-wall friction processes; 17 and (iii) in the case of granular material-based protective structures, shock energy is absorbed through a volumetric compaction/densification process. 22 Main objective.…”
Section: Introductionmentioning
confidence: 99%